Treatise on Materials Science and Technology, Volume 2; Volume 19, Part 1 |
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Page 17
DETECTOR X - RAY TUBE SOLLER SLIT SOLLER SLIT SPECIMEN POSITION
Fig . 7 . The parallel beam method . The dashed horizontal lines represent
various positions for the specimen . Note that since the angle between the
incident and ...
DETECTOR X - RAY TUBE SOLLER SLIT SOLLER SLIT SPECIMEN POSITION
Fig . 7 . The parallel beam method . The dashed horizontal lines represent
various positions for the specimen . Note that since the angle between the
incident and ...
Page 18
so IT for the error in peak shift at two tilts in degrees 20 , is 360 sin e 8 ( 420 ) sp =
— A ( 16 ) RGC Rp sin ( + ) ) ? where Rp represents the distance from the sample
to the focus position ; it is given by ( Hilley et al . , 1971 ) cos [ 4s + ( 90 - 0 ) ...
so IT for the error in peak shift at two tilts in degrees 20 , is 360 sin e 8 ( 420 ) sp =
— A ( 16 ) RGC Rp sin ( + ) ) ? where Rp represents the distance from the sample
to the focus position ; it is given by ( Hilley et al . , 1971 ) cos [ 4s + ( 90 - 0 ) ...
Page 160
temperature usually deviates very little from the bandgap position ( donor to
valence band transitions ) , due to the small donor binding energies associated
with the r conduction band minimum ( Bergh and Dean , 1976 ) . A relatively large
...
temperature usually deviates very little from the bandgap position ( donor to
valence band transitions ) , due to the small donor binding energies associated
with the r conduction band minimum ( Bergh and Dean , 1976 ) . A relatively large
...
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Contents
R JAMES | 2 |
Principles of XRay Stress Measurement | 4 |
Control of Accuracy and Precision | 25 |
Copyright | |
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absorption additional allows alloy angle Appl applications atoms bandgap beam broadening cause coefficients components composition composition profile concentration constant containing cooling crystal curve defects dependent deposits depth determined developed diffraction diffusion direction discussed dislocation distance distribution effect electron elements employed energy error et al example excitation experimental factor field function give given grain heat important included increasing intensity intensity bands iron laser lattice layer less magnetic material measurements Metals method Mössbauer observed obtained occur optical parameter peak phase Phys plane position possible powder problem produce range rays recent region relative residual stress sample semiconductors shift shown single Society solid spacing specimen spectra spectrum sputtering steel structure studies substrate surface target technique temperature term thickness values variation volume x-ray